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666 DYE-SENSITIZED SOLAR CELLS<br />

sheet resistance and high transparency. In addition, sheet resistance should be nearly<br />

independent of the temperature up to 500 ◦ C because sintering of the TiO 2 electrode is<br />

carried out at 450 to 500 ◦ C. Indium–tin oxide (ITO) is one of the most famous TCO<br />

materials. In spite of having low resistance at room temperature, ITO resistance increases<br />

significantly at high temperature in air. Usually, fluorine-doped SnO 2 is used as the TCO<br />

substrate for DSSCs (e.g. Nippon Sheet Glass Co., R = 8–10 /square).<br />

15.1.2.2 TiO 2 photoelectrode<br />

Photoelectrodes made of such materials as Si, GaAs, InP, and CdS decompose under irradiation<br />

in solution owing to photocorrosion. In contrast, oxide semiconductor materials,<br />

especially TiO 2 , have good chemical stability under visible irradiation in solution; additionally,<br />

they are nontoxic and inexpensive. The TiO 2 thin-film photoelectrode is prepared<br />

by a very simple process. TiO 2 colloidal solution (or paste) is coated on a TCO substrate<br />

and then sintered at 450 to 500 ◦ C, producing a TiO 2 film about 10 µm in thickness.<br />

Because this film is composed of TiO 2 nanoparticles (10–30 nm), giving it a nanoporous<br />

structure, the actual surface area of TiO 2 compared to its apparent surface area, roughness<br />

factor (rf), is >1000; that is, a 1-cm 2 TiO 2 film (10 µm thickness) has an actual surface<br />

area of 1000 cm 2 . The dye is considered to be adsorbed on the TiO 2 surface in a monolayer.<br />

Thus, if the nanoporous TiO 2 film has a high rf, the amount of dye adsorbed is<br />

drastically increased (on the order of 10 −7 mol cm −2 ), resulting in an increase of LHE that<br />

is near 100% at the peak absorption wavelength of the dye. In comparison, the amount<br />

of adsorbed dyes on the surface of single-crystal and polycrystal materials is quite small,<br />

with only 1% LHE even at the peak wavelength.<br />

Normally, the TiO 2 film contains large TiO 2 particles (250–300 nm), which can<br />

scatter incident photons effectively, to improve the LHE as shown later. The porosity<br />

of the film is also important because the electrolyte, which contains the redox ions,<br />

must be able to penetrate the film effectively to suppress the rate-determining step via<br />

diffusion of redox ions into the film. Appropriate porosity, 50 to 70%, is controlled in<br />

the sintering process by the addition of a polymer such as polyethylene glycol (PEG)<br />

and ethyl cellulose (EC) into the TiO 2 colloidal solution or paste. Figure 15.2 shows a<br />

scanning electron microscope (SEM) photograph of a typical nanocrystalline TiO 2 film. A<br />

detailed description of the procedure for preparing the TiO 2 film is given in Section 15.2.2.<br />

15.1.2.3 Ru complex photosensitizer<br />

The Ru complex photosensitizer, which contributes the primary steps of photon absorption<br />

and the consequent electron injection, is adsorbed onto the TiO 2 surface. The chemical<br />

structure of typical Ru complex photosensitizers developed by Grätzel’s group are<br />

shown in Figure 15.3 (TBA is tetrabutylammonium cation, (C 4 H 9 ) 4 N + ), and Figure 15.4<br />

shows absorption properties of the complexes in solution. The y-axis is represented by<br />

absorbance (A) and1− T(= 1 − 10 −A ),whereT is the transmittance. The cis-bis(4,4 ′ -<br />

dicarboxy-2,2 ′ -bipyridine)dithiocyanato ruthenium(II) (RuL 2 (NCS) 2 complex), which is<br />

referred to as N3 dye (or red dye), can absorb over a wide range of the visible<br />

regions from 400 to 800 nm. The trithiocyanato 4,4 ′ 4 ′′ -tricarboxy-2,2 ′ :6 ′ ,2 ′′ -terpyridine<br />

ruthenium(II) (black dye) (RuL’(NCS) 3 complex), absorbs in the near-IR region up to

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